{"title":"Comparison of a 1.1 kW-induction machine and a 1.5 kW-PMSM regarding common-mode bearing currents","authors":"M. Schuster, Janas Springer, A. Binder","doi":"10.1109/SPEEDAM.2018.8445298","DOIUrl":null,"url":null,"abstract":"An 1.1 kW-induction machine and an 1.5 kW-permanent magnet synchronous machine (PMSM) are investigated, measuring the common-mode bearing currents in dependence of rotor speed. Both machines are fed by an IGBT-voltage source inverter at $\\pmb{V}_{\\mathbf{DC}}=\\mathbf{560\\ V}$ DC link voltage. The parasitic high frequency machine capacitances are analytically calculated. The stator winding-to-frame capacitances are also measured. The 1.1 kW-induction machine shows at low speed $(\\pmb{n} < \\mathbf{900\\ rpm})$ resistive bearing currents, at medium speed (900 rpm $< \\pmb{n} < \\mathbf{2250}$ rpm) electrical discharge machining (EDM) bearing currents and at high speed above 2250 rpm capacitive dvldt bearing currents. The highest average peak-to-peak EDM bearing current is $\\pmb{I}_{\\mathbf{b},\\mathbf{pk}-\\mathbf{pk},\\mathbf{NDE}}\\approx 1$ A at non-drive end (NDE) and medium speed. With a Hertz'ian contact area $\\pmb{A}_{\\mathbf{Hertz}}=\\mathbf{0.21\\ mm}^{2}$ the apparent bearing current density $\\pmb{J}_{\\mathbf{b}}$ is 2.4 A/mm2• Thus it will probably reduce significantly the bearing life time. The 1.5 kW-PMSM shows mainly EDM bearing currents over almost the complete speed range $(\\mathbf{0} < \\pmb{n} < \\mathbf{3000}$ rprn $)$ with average peak-to-peak bearing currents of 0.1 A at drive end. The peak-to-peak bearing current of the resolver bearina is 300% higher. With a Hertz'ian contact area $\\pmb{A}_{\\mathbf{Hertz}}=\\mathbf{0.04\\ mm}^{2}$ the apparent bearing current density there is $\\pmb{J}_{\\mathbf{b}}=\\mathbf{4.7\\ A}/\\mathbf{mm}^{2}$. This high value will also reduce significantly the resolver bearing life time.","PeriodicalId":117883,"journal":{"name":"2018 International Symposium on Power Electronics, Electrical Drives, Automation and Motion (SPEEDAM)","volume":"75 1","pages":"0"},"PeriodicalIF":0.0000,"publicationDate":"2018-06-01","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":"9","resultStr":null,"platform":"Semanticscholar","paperid":null,"PeriodicalName":"2018 International Symposium on Power Electronics, Electrical Drives, Automation and Motion (SPEEDAM)","FirstCategoryId":"1085","ListUrlMain":"https://doi.org/10.1109/SPEEDAM.2018.8445298","RegionNum":0,"RegionCategory":null,"ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":null,"EPubDate":"","PubModel":"","JCR":"","JCRName":"","Score":null,"Total":0}
引用次数: 9
Abstract
An 1.1 kW-induction machine and an 1.5 kW-permanent magnet synchronous machine (PMSM) are investigated, measuring the common-mode bearing currents in dependence of rotor speed. Both machines are fed by an IGBT-voltage source inverter at $\pmb{V}_{\mathbf{DC}}=\mathbf{560\ V}$ DC link voltage. The parasitic high frequency machine capacitances are analytically calculated. The stator winding-to-frame capacitances are also measured. The 1.1 kW-induction machine shows at low speed $(\pmb{n} < \mathbf{900\ rpm})$ resistive bearing currents, at medium speed (900 rpm $< \pmb{n} < \mathbf{2250}$ rpm) electrical discharge machining (EDM) bearing currents and at high speed above 2250 rpm capacitive dvldt bearing currents. The highest average peak-to-peak EDM bearing current is $\pmb{I}_{\mathbf{b},\mathbf{pk}-\mathbf{pk},\mathbf{NDE}}\approx 1$ A at non-drive end (NDE) and medium speed. With a Hertz'ian contact area $\pmb{A}_{\mathbf{Hertz}}=\mathbf{0.21\ mm}^{2}$ the apparent bearing current density $\pmb{J}_{\mathbf{b}}$ is 2.4 A/mm2• Thus it will probably reduce significantly the bearing life time. The 1.5 kW-PMSM shows mainly EDM bearing currents over almost the complete speed range $(\mathbf{0} < \pmb{n} < \mathbf{3000}$ rprn $)$ with average peak-to-peak bearing currents of 0.1 A at drive end. The peak-to-peak bearing current of the resolver bearina is 300% higher. With a Hertz'ian contact area $\pmb{A}_{\mathbf{Hertz}}=\mathbf{0.04\ mm}^{2}$ the apparent bearing current density there is $\pmb{J}_{\mathbf{b}}=\mathbf{4.7\ A}/\mathbf{mm}^{2}$. This high value will also reduce significantly the resolver bearing life time.